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4.1.3.
Interference & Wave Nature of
Light <CJ chap 27 >
4.1.3.1.
Discussion
4.1.3.1.1.
Principle
of linear superposition: resultant disturbance is the sum of separate
disturbances
4.1.3.1.2.
Interference
is constructive if waves are in phase, destructive otherwise
4.1.3.1.3.
Thin
film interference described as with gasoline on water
4.1.3.1.4.
Diffraction
through a slit: resolving power is when the first dark band falls on the
central bright band
4.1.3.1.5.
Diffraction
grating – used to diffract light and create a spectroscope
4.1.3.2.
Mathematical
4.1.3.2.1.
Young’s
double slit experiment: sin q = m(l/d) constructive with m = 0, 1, 2; destructive m = 1/2 , 3/2..
4.1.3.2.2.
Thin
film lfilm = lvacuum /n and
4.1.3.2.2.1.
thus difference of distance =
2thickness + ½ lfilm (due to reflection) =½ lfilm , 3/2 lfilm…
4.1.3.2.2.2.
then subtracting ½ lfilm from each side one gets 2 t = 0, 1lfilm , 2lfilm , 3lfilm …
4.1.3.2.2.3.
then solving for t one gets t = m lfilm /2 where m = 0, 1, 2, 3, …
4.1.3.2.3.
Diffraction
through a single slit gives: sin q = m l /W where m = 1, 2, …,
W=width, for destructive intr
4.1.3.2.3.1.
qmin = 1.22 l/D for
the minimum resolution between two objects using an aperture D
4.1.3.2.3.2.
Diffraction grating maxima are sin q =
m l/d m = 1, 2, 3 where d is the slit separation
4.1.3.2.3.2.1.
red
is dispersed by the greatest angle and violet the least
4.1.3.3.
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